五 、新型說明： 【新型所屬之技術領域】 本創作係屬於發先- 叱一極體透鏡領域，特別是指 一種將中央集中之弁 寸⑺疋^ 避免直視時產生亮區之 域反町 之發先二極體透鏡改良結構。 【先前技術】V. New description: [New technology field] This creation belongs to the field of the first-polar lens, especially the one that concentrates the central concentration (7)疋^ The first diode lens improves the structure. [Prior Art]
按’發光二極體作A 股作為先源已然成為照明產業 發展趨勢，而將發井-权触 呆 —阁 先—極體之點光源轉換成為較大 範圍而均勻之出光，目丨丨失 _ 、J為發二極體照明發展之重 研究方向。將發光二極體與透鏡結合是一種可提古 照明效率且能有效轉換出光效果的方法，利用光： 折射、反射之基本原理，將發光二極體高功率之點 光源出光轉變成為柔和而均勾 J < ,，、'叨。—般使 發光二極體透鏡，大多可分成杯形、或半球體 形式’光線從發光二極體發射後’經過兩次 透鏡發射而出。杯形之發光二極體透鏡，係： 體側邊之全反射效應，使得光線往上方聚集形 勻之照明範圍，而半球體之發光二 句 U組遇鏡，則系 利用球體曲率造成光線折射效果，使得光線朝上’、 聚集’亦得到均勻之照明範圍。 方 此些設計雖能有效改變發光二極體之出光 光線能夠均勻照設於固定範圍之照明區域，伸== 去避免中心區域較明亮而越外圈越昭 ··'、 ,、、、π效果， M432143 使得人眼直視仍可辨識出下方之發光二極體光源。 除此之外’杯體側面曲面以及半球體曲面多為平滑 設計’但造成在同樣的視角下人眼直視時，僅有一 固定區域之光線照射該視角方向而造成視覺上之亮 塊出現。此等缺失使得現有之發光二極體透鏡雖能 提供均勻之出光及照明，但仍無法使得發光二極體 成為人眼可直視之照明燈具。請參考美國公告號 US201 1/01 57898A1之專利，係提供一種改變出光方 向使得光線涵蓋360度出光方向之透鏡，以及台灣 公告號1 262604之專利，係提供一種將出光導向側 面或背面之透鏡。此兩種透鏡之設計皆能將中央出 光之光線導向側面或是其它角度，而產生均勻散光 之光學效果，由於其入光面與光線行徑方向皆近乎 垂直’故往正面方向之光源近無改變方向仍然直射 至出光面，方經過出光面之折射而改變方向，但由 於入光角度會影響產生拼糾μ θ 王斫射與反射之光量，故其光 學效果仍受到極大之侷限。 、 柯喂。此外，該等設計仍無法 改善肉眼直視時，同—鉬β α 視角所見透鏡提供之光線仍 為一亮區及其它暗區。 是故，有鑑於上述 &缺失’本創作係提供一種能According to the 'light-emitting diodes as the A-shares as the precursor, it has become the development trend of the lighting industry, and the point source of the well-right touch--the first-polar body is converted into a larger range and uniform light, and the target is lost. _, J is the research direction of the development of diode lighting. The combination of the light-emitting diode and the lens is a method for improving the illumination efficiency and effectively converting the light effect, and using the basic principle of light: refraction and reflection, the light source of the high-power light source of the light-emitting diode is converted into a soft and uniform light. Hook J < ,,, '叨. Generally, the light-emitting diode lens can be mostly divided into a cup shape or a hemispherical form. After the light is emitted from the light-emitting diode, it is emitted through two lenses. The cup-shaped light-emitting diode lens is a full-reflection effect on the side of the body, so that the light illuminates the uniform illumination range upwards, and the light-emitting two-segment U-group of the hemisphere is reflected by the curvature of the sphere. The effect is that the light is directed 'up' and 'aggregated' to obtain a uniform illumination range. Although these designs can effectively change the light output of the light-emitting diodes, they can be uniformly illuminated in the fixed area of the illumination area. Extension == to avoid the brighter central area and the outer circle is more ···,,,,, π The effect, M432143 allows the human eye to still recognize the underlying LED source. In addition, the 'side surface of the cup and the surface of the hemisphere are mostly smooth design', but when the human eye is directly viewed from the same angle of view, only a fixed area of light illuminates the viewing angle to cause a visually bright block. These defects make the existing light-emitting diode lens provide uniform light and illumination, but still cannot make the light-emitting diode become a lighting fixture that can be directly viewed by the human eye. Please refer to the U.S. Patent Publication No. US 201 1/01 57898 A1, which is incorporated herein by reference in its entirety, the entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all all Both lenses are designed to direct the light from the center to the side or other angles, resulting in an optical effect of uniform astigmatism. Since the light-incident surface is nearly perpendicular to the direction of the light, the light source in the front direction has not changed. The direction is still directly to the light-emitting surface, and the direction is changed by the refraction of the light-emitting surface. However, since the light-input angle affects the amount of light that causes the shot and reflection, the optical effect is still greatly limited. Ke feeds. In addition, the design still does not improve the direct view of the naked eye, and the light provided by the lens from the perspective of the molybdenum β α is still a bright area and other dark areas. Therefore, in view of the above & missing, this creative department provides a kind of
有效避免光線集中於中奂F 一 为&域，以及人眼直視時造 成亮區之發光二極體透鐘 兄改良結構，使得燈具提供 使用時肉眼直視時光線更 不尺加舒適均勻。 4 M432143 【新型内容】 本創作之主要目的，旨在提供一種壁面光線集 中於中央而照度均勻，且人眼直視時避免產生亮區 之發光二極體透鏡改良結構。 為達上述目的，本創作之發光二極體透鏡改良 結構，供以與一發光二極體光源結合以改善出光效 果’該發光二極體透鏡改良結構具有一本體，係為 截頂圓錐狀體並以一中央軸心線呈現軸對稱，該本 體之錐頂凹設形成有一入光面，該本體之錐底形成 有一出光面，該本體之側壁則形成有一光學曲面， 該發光二極體透鏡改良結構，其特徵在於：該本體 之該入光面係收束成形於一第一發散點，且該第一 發散點係位於該中央軸心線位置，又該光學曲面上 係形成一多區域反射結構，據以將從入光面進入該 本體之光線均勻分佈由該出光面射出，以避免整片 之亮區造成視覺效果上之不平均，該多區域反射結 構係為複數個網格結構，且各該網格結構之側剖面 為直線或平滑曲線，邊框則分別呈四邊形或六邊 形。而為了加強反射之功效，該發光二極體透鏡改 良結構更包含一反射層.，係設於該本體外側並僅包 覆該光學曲面及該等網格結構。 為了加強分散中央區域光線之效果，該出光面 係收束成形於一第二發散點’且該第二發散點係位 於該中央軸心線位置而相對該第一發散點位置設 5 置’使得光線分佈更加平均。 而為使該發光二極體透鏡改良結構便於使用， 其更包含至少一安裝構件’設於該本體之錐頂、錐 底' 或兩者兼具。 為前述之目的’本創作亦提供一種發光二極體 透鏡改良結構’供以與一發光二極體光源結合以改 善出光效果，該發光二極體透鏡改良結構具有一本 體’係為截頂圓錐狀體並以一中央軸心線呈現軸對 稱’該本體之錐頂凹設形成有一入光面，該本體之 錐底形成有一出光面’該本體之側壁則形成有一光 學曲面’該發光二極體透鏡改良結構，其特徵在於： 該本體之該出光面係收束成形於一第二發散點，且 該第二發散點係位於該中央轴心線位置，又該光學 曲面上係形成一多區域反射結構’據以將從入光面 進入該本體之光線均勻分佈由該出光面射出，以避 免整片之売區造成視覺效果上之不平均，該多區域 反射結構係為複數個網格結構，且各該網格結構之 側剖面為直線或平滑曲線。而為了加強反射之功 效’該發光二極體透鏡改良結構更包含一反射層， 係設於該本體外側並僅包覆該光學曲面及該等網格 結構。 為達前述目的，本創作更提供一種發光二極體 透鏡改良結構’供以與一發光二極體光源結合以改 善出光效果，該發光二極體透鏡改良結構具有一本 6 狀:並"央……對 錐底形成有一出：°又：成有-入光面，該本體之 學曲面，节發朵 本體之側壁則形成有-光 該光學曲面上=體透㈣良結構，其特徵在於: 形成一多區域反射結構，據以將從 /入該本體之光線均勻分佈由該出光面射 =避免整片之亮區造成視覺效果上之不平均， 二夕£域反射結構係為複數個網格結構，且各該網 結構之側剖面為直線或平滑曲線，邊框則分別呈 四邊形。而為了加強反射之功效，該發光二極體透 文良、。構更包含_反射層，係設於該本體外側並 僅包覆該光學曲面及該等網格結構。 透過上述之設計，可將中央區域直射之光線經 由入光面而折射往不同角度’而有效避免光線集中 於中央區$，使得點光源之發光二極體經由透鏡轉 換後，變成均勻之照度分佈。同時該多區域反射結 構能將光線分散由不同區域之結構反射至同一視 角，避免人眼直視時因為平滑之反光區域產生整片 之亮區而不舒適，進而使得燈具提供使用時肉眼直 視時光線更加舒適均勻。. 【實施方式】 為使貴審查委員能清楚了解本創作之内容，謹 以下列說明搭配圖式，敬請參閱。 言月參閱第1圖，係為本創作較佳實施例之立體 外觀圖。如圖中所示，本創作提供之發光二極體透 鏡改良結構具有一本體i，係為截頂圓錐狀體，並 以一中央軸心線2呈現軸對稱，該本體i之錐頂凹 a又形成有一入光面1〇，使光線經由該入光面丨〇進 入該本體1，並於進入該本體丨時產生折射。該本 體1之錐底形成有一出光面12，使光線經由該出光 面12離開該本體卜提供照明等功用。該本體1之 側壁則形成有一光學曲面丨4，該光學曲面丨4描述 形成該本體1之錐狀體侧面弧度、曲率、椎狀體高 度等外型，提供該發光二極體透鏡改良結構之主要 之光干效果。該發光二極體透鏡改良結構之特徵在 於該本體1之該入光面10係收束成形於一第一發散 點1 00 ’且該第一發散點丨〇〇係位於該中央軸心線2 位置使得該第一發散點1 0 0位於光線直射之路徑 上，以使光線從該第一發散點100進入該本體1時 f生偏折造成折射，降低直線進入該本體1之光線 量。又該光學曲面14上係形成-多區域反射結構 140，據以將從入光面1〇進入該本體i之光線經由 該多區域反射結構140均勻分佈由該出光面12射 出，避免產生大面積之亮區。該多區域反射結構140 f為複數個網袼結構1401，該等網格結構之 單、揭格外觀可為四邊形或六邊形’本實施例中各 該網格外觀係為四邊形，由該本體i之錐頂彼此鄰 8 M432143 接佈設裏該本體1之錐底，使得該等網格結構ΐ4〇ι 之邊緣形成從該本體1之錐頂延伸至錐底之轄射 線，及以該中央軸心線2為圓心之複數個同心圓交 又而成之大小漸增之方格，且該等網格結構14〇1中 之側剖面為直線或平滑曲線，以提供不同之光線反 射效果。 請參閲第2a〜2d圖，係為本創作第一實施例之 不同態樣之剖面圖。如圖中所示，該等網格結構ΐ4〇ι 之側剖面為朝外凸出之平滑曲線，彼此相連而形成 整體為波浪狀之該多區域反射結構14〇。該入光面 10之曲率及外觀係與該光學曲面14互相搭配輔 助，以提供最佳之照明效果，由於光之性質，由光 疏之介質進入光密之介質時，不會發生全反射現 象，故於此端進行設計能軚為有效而容易提升折射 光線之效果，而不會因為光線反射而增加光學設計 上之複雜度。以直射進入透鏡之光線路徑討論之， 如2a圖所示，該入光面1〇之斜率變化使得直射進 入該本體1.之光線在該入光面1〇中央區域產生大角 度之偏折，而在該入光.面1〇邊緣區域則產生較小角 度之偏折，因而使得照射到該光學曲面14之光量提 升如2b圖所不，該入光面10之斜率固定使得直 射進入該本體1之光線均勻朝向固定角度產生偏 折L較2a圖中之中央區域之光線偏折角度較小，對 於亮度較低之光源可避免該入光面1〇中央區域光 9 線過度發散而造成暗區。 ZC圖所不，該入光面 1 0係以兩段不同之斜率所 ^ ^ 傅风〒央區域之光線偏 折角度較2b圖中更小，而々k 丨> , 而外側之光線偏折角度則較It effectively prevents the light from being concentrated in the middle and the F, and the light-emitting diodes that make the bright areas in the direct view of the human eye improve the structure, so that the light is provided with a lighter and more uniform light when viewed directly. 4 M432143 [New content] The main purpose of this creation is to provide an improved structure of a light-emitting diode lens in which the wall light is concentrated in the center and the illumination is uniform, and the human eye is directly viewed to avoid bright areas. In order to achieve the above object, the improved structure of the light-emitting diode lens of the present invention is combined with a light-emitting diode light source to improve the light-emitting effect. The improved structure of the light-emitting diode lens has a body and is a truncated cone. And the axis of the central axis is axisymmetric, the cone top of the body is concavely formed with a light incident surface, the cone bottom of the body is formed with a light emitting surface, and the sidewall of the body is formed with an optical curved surface, the light emitting diode lens The improved structure is characterized in that: the light incident surface of the body is bundled and formed at a first divergence point, and the first divergent point is located at the central axis line position, and the optical curved surface forms a multi-region The reflecting structure is configured to uniformly distribute the light entering the body from the light incident surface from the light exiting surface to avoid the visual effect unevenness caused by the bright area of the whole piece, and the multi-region reflective structure is a plurality of mesh structures. And the side profile of each of the grid structures is a straight line or a smooth curve, and the borders are respectively quadrilateral or hexagonal. In order to enhance the effect of reflection, the light-emitting diode lens improved structure further comprises a reflective layer disposed outside the body and covering only the optical curved surface and the mesh structure. In order to enhance the effect of dispersing the light in the central region, the light exiting surface is formed at a second divergence point 'and the second divergent point is located at the central axis line position and is set to 5 with respect to the first divergence point position. The light distribution is more even. In order to make the improved structure of the light-emitting diode lens easy to use, it further comprises at least one mounting member 'provided on the top of the cone, the bottom of the cone' or both. For the purpose of the foregoing, the present invention also provides an improved structure of a light-emitting diode lens for combining with a light-emitting diode light source to improve the light-emitting effect. The improved structure of the light-emitting diode lens has a body 'system as a truncated cone The body is axially symmetric with a central axis. The cone top of the body is recessed to form a light incident surface, and the cone bottom of the body is formed with a light exit surface. The sidewall of the body is formed with an optical curved surface. The improved structure of the body lens is characterized in that: the light-emitting surface of the body is bundled and formed at a second divergence point, and the second divergence point is located at the central axis line position, and the optical surface is formed by a plurality of The regional reflection structure is configured to uniformly distribute the light entering the body from the light incident surface from the light exit surface to avoid visual unevenness in the entire region, and the multi-region reflective structure is a plurality of meshes. Structure, and the side profile of each of the mesh structures is a straight line or a smooth curve. In order to enhance the effect of reflection, the improved structure of the light-emitting diode lens further comprises a reflective layer disposed outside the body and covering only the optical curved surface and the mesh structure. In order to achieve the above purpose, the present invention further provides an improved structure of a light-emitting diode lens for combining with a light-emitting diode light source to improve light-emitting effect. The improved structure of the light-emitting diode lens has a shape of 6: and " The central part of the cone is formed with a cone: the bottom surface is formed into a light-incident surface, and the curved surface of the body is formed on the side wall of the body, and the optical surface is formed on the optical surface (the body is transparent). The method comprises: forming a multi-region reflection structure, according to which the light from the body is evenly distributed from the light-emitting surface = avoiding the unevenness of the whole film to cause visual unevenness, and the reflection structure of the second-phase domain is plural Grid structure, and the side profile of each mesh structure is a straight line or a smooth curve, and the borders are respectively quadrangular. In order to enhance the effect of reflection, the light-emitting diode is transparent. The structure further includes a reflective layer disposed outside the body and covering only the optical curved surface and the mesh structures. Through the above design, the direct light in the central region can be refracted to different angles through the light incident surface to effectively prevent the light from being concentrated in the central region $, so that the light emitting diode of the point light source is converted into a uniform illumination distribution after being converted by the lens. . At the same time, the multi-region reflective structure can reflect the light dispersion from the structure of different regions to the same viewing angle, avoiding the unsightly appearance of the entire bright region due to the smooth reflective region when the human eye is directly viewed, thereby enabling the light to be directly viewed by the naked eye when the light is used. More comfortable and even. [Embodiment] In order to make your reviewer understand the content of this creation, please refer to the following description. Referring to Figure 1, it is a three-dimensional appearance of the preferred embodiment of the present invention. As shown in the figure, the improved structure of the LED lens provided by the present invention has a body i which is a truncated cone and exhibits axis symmetry with a central axis 2, and the cone a of the body i A light entrance surface 1 又 is formed to allow light to enter the body 1 through the light entrance surface and to refract when entering the body 丨. The cone bottom of the body 1 is formed with a light-emitting surface 12 for allowing light to exit the body via the light-emitting surface 12 to provide illumination and the like. An optical surface 丨4 is formed on the sidewall of the body 1. The optical curved surface 描述4 describes the shape of the side of the cone of the body 1 such as curvature, curvature, height of the vertebral body, etc., and provides an improved structure of the illuminating diode lens. The main light dry effect. The improved structure of the LED lens is characterized in that the light incident surface 10 of the body 1 is bundled and formed at a first divergence point 100 ' and the first divergence point is located at the central axis 2 The position is such that the first divergence point 100 is located on the path of the direct light so that the light is deflected from the first divergence point 100 into the body 1 to cause refraction, reducing the amount of light entering the body 1 by the straight line. Further, the optical curved surface 14 is formed with a multi-region reflective structure 140, whereby light rays entering the body i from the light incident surface 1 are uniformly distributed through the multi-region reflective structure 140, and are emitted from the light-emitting surface 12, thereby avoiding a large area. Bright area. The multi-region reflective structure 140 f is a plurality of mesh structures 1401. The single and uncovered appearances of the mesh structures may be quadrilateral or hexagonal. In this embodiment, the mesh appearance is a quadrilateral. The cone tops of i are adjacent to each other 8 M432143, and the bottom of the body 1 is arranged such that the edges of the mesh structures 形成4〇ι form a ray from the cone top of the body 1 to the bottom of the cone, and the central axis The heart line 2 is a square of increasing and increasing size of a plurality of concentric circles of the center, and the side profiles of the mesh structures 14〇1 are straight lines or smooth curves to provide different light reflection effects. Referring to Figures 2a to 2d, there are shown cross-sectional views of different aspects of the first embodiment of the present invention. As shown in the figure, the side profiles of the grid structures 为4〇ι are smooth curves that protrude outward, and are connected to each other to form the multi-region reflecting structure 14〇 which is entirely wavy. The curvature and appearance of the light-incident surface 10 are matched with the optical curved surface 14 to provide an optimal illumination effect. Due to the nature of the light, the total reflection phenomenon does not occur when the light-diffusing medium enters the optically dense medium. Therefore, the design at this end can be effective and easy to enhance the effect of refracting light without increasing the complexity of optical design due to light reflection. As discussed in the light path of the lens entering the lens, as shown in FIG. 2a, the slope of the light incident surface 1〇 causes the light entering the body 1. to generate a large angle deflection in the central region of the light incident surface. In the edge region of the light incident surface, a small angle is generated, so that the amount of light irradiated to the optical curved surface 14 is increased as shown in FIG. 2b, and the slope of the light incident surface 10 is fixed so that the light enters the body directly. The light of 1 is evenly deflected toward the fixed angle. The deflection angle of the light is smaller than that of the central region of the 2a image. For the light source with lower brightness, the light 9 of the central region can be prevented from being excessively diverged and dark. Area. The ZC map does not, the light-incident surface 10 is separated by two different slopes. ^ The wind deflection angle of the Fufeng 〒 area is smaller than that of the 2b diagram, and 々k 丨> Fold angle
大’使得該入光面10中本F Y夹區域直射光線之折射效果 較輕微而邊緣區域之折射齡或 _ 外耵1乂為明顯。此外如2d圖所 示’該入光面1 0係以—段田— 丰又固疋斜率以及一段曲面所 形成’使得進入該本體1 之光線折射產生局部性更 加細微之變化，使得光學寺罢 T兀子效果更加精緻。除了上述 之實施樣態，該入光面10之形狀以及光學設計更可 細分成多段曲率、或者是各部分產生高低'凹凸之 局部結構’增加或是降低光之折射效果，搭配該光 學曲面14之設計以達成最佳之照明功效以及視覺 感受。 請一併參閱第3a ' 3b圖，係為本創作多區域反 射結構之兩種示意圖。如圖中所示，該多區域反射 結構140係為複數個網格結構14〇1 ’各該網格結構 1401之側剖面均為平滑之曲面，如第圖所示， 該等網格結構1401之側剖面係為朝外凸出之平滑 曲面，由於每個該等網格結構14〇1皆有相似之曲 面，故當肉眼在與該出光面12垂直方向正視該出光 面1 2時’光線分別由該等網格結構14 〇 1之一邊反 射至同一視角，如圖中「」之光線示意。故在人 眼'上並非呈現整片之亮面，而是分別置於該等網格 結構1401 —部份之小亮面。應注意的是，由於該等 10 該多區域反射結構140係供以將光線反射至該出光 面12*故於設計時需考量光線全反射之效應，各該 網格結構1 401之曲面各係使光線之入射角度大於 全反射之臨界角（臨界角θε =透鏡折射率D之正弦 反函數sinll/D))，以降低從該光學曲面14折射 而散逸之光線量。此外，為了加強反射之功能，使 得反射至該出光面12之光量增加，該多區域反射結 構140更包含一反射層16，設於該本體1外側並僅 包覆該光學曲面14及該等網格結構1401，該反射 層16可塗佈金屬、PP或PET等高反射率之材質， 避免進入該本體1之光線從該光學曲面14穿出該本 體1，轉而因接觸該反射層16而反射至該出光面 12，因而增加出光量以提升亮度。 同理’在侧視該出光面1 2時，亦由該等網格結 構14 01之一部份反射至該視角。如此之設計不僅能 夠免除整面之亮暗區而提升肉眼直接注視時之柔和 感’而且由於該光學曲面14之外型因為該多區域反 射結構1 40而變化，因而使得能夠反射到同一視角 之區域遍布該光學曲面1 4非僅偈限於一區域，辱而 使得視覺上更加均勻。而第3b圖中所示為該等網格 結構1 4 01之側剖面係為朝内凹入之平滑曲面，其與 第3a圖之外凸結構有類似而相反之效果，兩者於相 同視角所見之該等網格結構14 〇 1之發亮區域位置 相反，以肉眼正視該出光面丨2之視角為例（圖中 M432143 -->j之光線），第3a圖中之光線反射區域為該 等網格結構1401遠離該出光面12處，而第3b圖中 之光線反射區域則為該等網格結構14〇1靠近該出 光面12處。雖然凹凸兩種該等網格結構1 4 〇 i同一 視角之反射區域不同，但均可提供該發光二極體透 鏡改良結構光線均勻之效果。 另請參閱第4、5圖，係為本創作第二實施例之 立體外觀圖及剖面示意圖。如圖中所示，該發光二 極體改良結構之該出光面i 2係收束成形於一第二 發散點120，以加強中央區域之光線折射之效果， 且該第二發散點120係位於該中央軸心線位置而相 對該第一發散點100位置設置。當光線由該本體丄 經由該多區域反射結構丨4〇 (如圖中所示，為剖面 朝該本體1凹設之該等網格結構1401)而接觸該出 光面12時，將產生第二次之折射作用，因而使 線再次產生偏折。由於該入光面1〇、該光學曲面Η 皆有均勻光線之效果，該出光面12之結構設計可對 出光之效果作進-步之修正，對於局部或係為之光 線效果加以改良，而使光線分佈更加均勻值得一 提的是，該多區域反射結冑140 1不侷&於相同樣 式結構之網格結構，亦可由不規則之多邊形組合而 成，透過該多區域反射結構140之不規則設計使得 反射之光線路徑較不規則，因而提高出光之均勻产。 另請參閱第6圖’係為本創作之實施示意二。 12 如圖中所示’該發光_ 安裝構件3，設於該本：體改良結構更包含至少一 或兩者兼具，以便於裝执__之雜頂 '該本體之錐底、 將該發光二極體改良二：發光二極體光源4’並 未顯示）上。 、、構震設於使用之燈具（圖中 另請參閱第7a及m .. 圖，係為本創作第=森 例之立體外觀圖及剖 』卞弟一只施 .,,^ 不思圖。本創作另提供不同 手&以達到散光均勻 效果，如圖中所示，發光-極體透鏡改良結構具有截頂圓錐狀之一本體7: 中央軸。線2呈軸對稱’該本體7之錐頂凹設 形成有一入光面7°’供以容置該發光二極體光源 4並使光線經由該入光面70進入該本體7。該本 體7之錐底形成有一出光面72，且其特徵在於該出 光面72係收束成形於一第二發散點72〇，且該第二 發散點720係位於該中央軸心線2，之位置使光 線直射進入該本體7後，經由從該第二發散點7 2 〇 產生偏折造成折射，降低直線射出該本體7之光線 置。該本體7之側壁則為一光學曲面74，以描述該 本體7之錐狀側面弧度、曲率、椎狀體高度等外型， 且其特徵在於該光學曲面74上形成一多區域反射 結構740，據以將從入光面70進入該本體7之光線 經由該多區域反射結構740均勻分佈由該出光面72 射出’避免產生大面積之亮區。該多區域反射結構 740係為複數個網格結構7401，於本實施例中，各 M432143 該網格結構7 4 01係為六邊创 p* &細 q/、透型，形彼此鄰接形成蜂巢 狀並由該本體7之錐頂你μ 5雜虎 戸J貝师6又至錐底’且各該網格結 構7401之側剖面為直線或平滑曲線，以提供不同之 光線反射效果。於此結構中，光線從該入光面7〇進 入該本冑7時產生—次折射而照射至該多區域反射 結構740,而在該等網格結構74〇1之曲線或直線邊 緣產生反射，因而將光線散佈至不同視角，另，一 次折射角度不大而從該入光面7〇直射至該出光面 72之光線，則透過該出光面72枚束至該第二發散 點720之設計，使得光線往邊緣折射因而使得光線 分佈更加均勻。且為了加強反射之功能，使得反射 至該出光面72之光量增加，該發光二極體透鏡改良 結構更包含一反射層76，以金屬、PP或PET等高反 射率之材質设於該本體1外側並僅包覆該光學曲面 74及該等網格結構7401，降低從該光學曲面74折 射出該本體7之光線量，轉而因接觸該反射層76而 反射至該出光面72’因而增加出光量以提升亮度。 另請參閱第8a及8b圖，係為本創作第四實施 例之立體外觀圖及剖面示意圖。本創作另針對不同 發光型態之一發光一極體光源4 ”提供不同手段以 達到散光均勻之效果’如圖中所示，該發光二極體 透鏡改良結構亦具有截頂圓錐狀之一本體8，以一 中央轴心線2”呈轴對稱，於該本體8之錐頂凹設 形成有一入光面80’供以容置該發光二極體光源 14 M432143 4並使光線經由該入光面80進入該本體8,並由 該本體8錐底之一出光面82發散產生照明效果。該 本體8之側壁為一光學曲面84，以描述該本體8之 錐狀側面弧度、曲单、椎狀體高度等外型，且其特 徵在於該光學曲面84上形成一多區域反射結構 840，據以將從入光面8〇進入該本體8之光線經由 該多區域反射結構840均勾分佈由該出光面82射The large size makes the refractive effect of the direct ray of the FF region in the light-incident surface 10 slightly lighter and the refracting age of the edge region or _ 耵1乂 is obvious. In addition, as shown in Fig. 2d, the light-incident surface of the light-incident surface is formed by the slope of the segment and the surface of the curved surface, so that the light entering the body 1 is refracted to produce a more subtle change in locality. The dice effect is more refined. In addition to the above-described implementation, the shape and optical design of the light-incident surface 10 can be subdivided into a plurality of segments of curvature, or each portion produces a high or low 'local structure of the bumps' to increase or decrease the refractive effect of the light, with the optical curved surface 14 Designed for optimal lighting and visual experience. Please refer to the 3a '3b diagram together for the two schematic diagrams of the multi-regional reflection structure. As shown in the figure, the multi-region reflective structure 140 is a plurality of mesh structures 14 〇 1 'the side profiles of each of the mesh structures 1401 are smooth curved surfaces, as shown in the figure, the mesh structures 1401 The side profile is a smooth curved surface that protrudes outward. Since each of the mesh structures 14〇1 has a similar curved surface, when the naked eye is facing the light exiting surface 1 2 in a direction perpendicular to the light exiting surface 12, the light is The light is reflected from one side of the grid structure 14 〇1 to the same viewing angle, as indicated by the light in the figure. Therefore, the whole face is not presented on the human eye, but is placed on the small glossy surface of the mesh structure 1401. It should be noted that since the multi-region reflective structure 140 is configured to reflect light to the light-emitting surface 12*, the effect of total light reflection needs to be considered in design, and the curved surfaces of each of the mesh structures 1 401 The incident angle of the light is made larger than the critical angle of total reflection (critical angle θ ε = sinusoidal inverse function sinll/D of the lens refractive index D)) to reduce the amount of light escaping from the optical curved surface 14 to dissipate. In addition, in order to enhance the function of the reflection, the amount of light reflected to the light-emitting surface 12 is increased. The multi-region reflective structure 140 further includes a reflective layer 16 disposed outside the body 1 and covering only the optical curved surface 14 and the nets. In the lattice structure 1401, the reflective layer 16 can be coated with a material having a high reflectivity such as metal, PP or PET, so that light entering the body 1 can be prevented from passing through the optical surface 14 from the body 1 and in turn contacting the reflective layer 16. Reflected to the light exit surface 12, thereby increasing the amount of light to enhance the brightness. Similarly, when the light exit surface 1 2 is viewed sideways, a portion of the mesh structures 14 01 is also reflected to the viewing angle. Such a design not only eliminates the bright and dark areas of the entire surface but enhances the soft feeling when the naked eye directly gazes 'and because the optical curved surface 14 is changed by the multi-region reflective structure 140, thereby enabling reflection to the same viewing angle. The area throughout the optical surface 14 is not limited to only one area, which makes the visually more uniform. And the side profile of the grid structure 1 4 01 is a smooth curved surface that is concave inward, which has a similar and opposite effect to the convex structure of the 3a figure, both of which are at the same angle of view. As seen, the positions of the bright areas of the grid structures 14 〇 1 are opposite, and the angle of view of the light exit surface 丨 2 is visually recognized as an example (the light of M432143 -->j in the figure), and the light reflection area of the 3a picture The grid structure 1401 is away from the light exit surface 12, and the light reflection area in Fig. 3b is such that the grid structure 14〇1 is close to the light exit surface 12. Although the concave and convex views of the two mesh structures 1 4 〇 i are different from the same viewing angle, the light-emitting diode lens can be provided to improve the uniform light structure. Please also refer to Figures 4 and 5 for a perspective view and a cross-sectional view of the second embodiment of the present invention. As shown in the figure, the light-emitting surface i 2 of the improved structure of the light-emitting diode is constricted and formed at a second divergence point 120 to enhance the effect of light refraction in the central region, and the second divergent point 120 is located. The central axis position is set relative to the first divergence point 100. When the light is contacted by the body 丄 via the multi-region reflective structure 〇4〇 (the grid structure 1401 is recessed toward the body 1 as shown in the figure), the second light surface 12 will be produced. The second refraction causes the line to deflect again. Since the light-incident surface 1〇 and the optical surface Η have the effect of uniform light, the structure of the light-emitting surface 12 can be corrected for the effect of the light-emitting, and the light effect of the local or the system is improved. To make the light distribution more uniform, it is worth mentioning that the multi-region reflection structure 140 1 is not in the same mesh structure of the same pattern structure, and may also be composed of irregular polygons, and the multi-region reflection structure 140 is Irregular design makes the reflected light path more irregular, thus improving the uniform output of light. Please also refer to Figure 6 for the implementation of the second creation. 12 as shown in the figure, the 'lighting_mounting member 3 is disposed in the body: the body-improved structure further comprises at least one or both, so as to facilitate the mounting of the __ The light-emitting diode is improved two: the light-emitting diode light source 4' is not shown). , and the structure of the damper is used in the lighting (see also the 7a and m.. in the figure, which is the three-dimensional appearance and section of the creation of the second example). The creation also provides different hands & to achieve astigmatism uniformity, as shown in the figure, the illuminating-polar lens improved structure has a truncated cone-shaped body 7: central axis. Line 2 is axisymmetric 'the body 7 The cone top recess is formed with a light incident surface 7°' for receiving the light emitting diode light source 4 and allowing light to enter the body 7 via the light incident surface 70. The cone bottom of the body 7 is formed with a light exit surface 72. The light-emitting surface 72 is convergently formed at a second divergence point 72〇, and the second divergence point 720 is located at the central axis line 2, and the light is directly incident into the body 7 through the slave. The second divergence point 7 2 〇 is deflected to cause refraction, and the light of the straight line is emitted from the body 7. The side wall of the body 7 is an optical curved surface 74 to describe the tapered side curvature, curvature, and vertebra of the body 7. a shape such as a height of the body, and characterized in that a multi-region is formed on the optical curved surface 74 The radiation structure 740 is configured to uniformly distribute the light entering the body 7 from the light incident surface 70 through the multi-region reflective structure 740 from the light exit surface 72 to avoid a bright area of a large area. The multi-region reflective structure 740 is a plurality of mesh structures 7401. In the present embodiment, each M432143 mesh structure 7 4 01 is a hexagonal p* & fine q/, transmissive, and the shapes are adjacent to each other to form a honeycomb shape and are formed by the body 7 The cone tops you μ 5 戸 戸 贝 贝 贝 贝 贝 贝 贝 贝 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 且 740 740 740 740 740 740 When the light surface 7〇 enters the local 胄7, a secondary refraction is generated to illuminate the multi-region reflective structure 740, and a reflection is generated at a curved line or a straight edge of the mesh structure 74〇1, thereby spreading the light to different viewing angles. In addition, the light having a small refraction angle from the light incident surface 7 to the light exit surface 72 is transmitted through the light exit surface 72 to the second divergence point 720, so that the light is refracted toward the edge and the light is made More evenly distributed, and in order to strengthen the anti The function of the shot is such that the amount of light reflected to the light-emitting surface 72 is increased. The improved structure of the light-emitting diode lens further comprises a reflective layer 76, which is disposed outside the body 1 with a material having high reflectivity such as metal, PP or PET and only The optical curved surface 74 and the mesh structure 7401 are covered to reduce the amount of light that is refracted from the optical curved surface 74, and then reflected to the light-emitting surface 72' by contacting the reflective layer 76, thereby increasing the amount of light. Please also refer to Figures 8a and 8b, which are perspective views and cross-sectional views of the fourth embodiment of the present invention. The present invention provides different means for different light-emitting type one-pole light source 4" The effect of uniform astigmatism is as shown in the figure. The improved structure of the LED lens also has a truncated cone-shaped body 8 which is axisymmetric with a central axis 2", and the cone of the body 8 is concave. A light-emitting surface 80' is formed to receive the light-emitting diode light source 14 M432143 4 and the light enters the body 8 via the light-incident surface 80, and is diverged by the light-emitting surface 82 of the cone bottom of the body 8 to generate illumination. effect. The side surface of the body 8 is an optical curved surface 84 for describing the shape of the tapered side curvature, the curved piece, the height of the vertebral body, and the like, and is characterized in that a multi-region reflective structure 840 is formed on the optical curved surface 84. According to the multi-region reflective structure 840, the light entering the body 8 from the light-incident surface 8 is distributed by the light-emitting surface 82.
出，避免產生大面積之亮區。該多區域反射結構84〇 係為複數個網格結構8401，於本實施例中，各該網 格結構840 1為另一種六邊形’彼此鄰接成為如羽毛 格狀由該本體8之錐頂佈設至錐底，且各該網格結 構840 1之側剖面為直線或平滑曲線，當該發光二極 體光源4”為亮度較低，或由二顆以上之發光二極 體組成，使得該發光二極體光源4”所發散之光線 並非集中於一亮點，故中央區域母須特別提供散光 之構造而照射至該多區域反射結構84〇在該等網 格結構84〇1之曲線或直線邊緣產生反射，因而將光 線散佈至不同視角，而避免單—视角產生亮區之情 形。且為了降低從該光學曲面84折射出該本體8之 光線量’使得反射至該出光面82之光量增加，該發 光二極體透鏡改良結構更包含一反射層86，設於該 本體1外側並以金屬、PP或PET等高反射率之材質 包覆該光學曲面84及該等網格結構84〇1，因而增 加出光量以提升亮度。 15 M432143 綜上所述’本創作在實施時，能有 鏡之光線折射至不同之角度，大幅降低 極體點光源之高亮度直射及邊緣之照度 經過透鏡之出光呈現整面均勻之亮度。 之收束設計不僅有效改良光線折射角度 效果顯著’更辅以出光面之設計，使得 度更加提升。而透鏡之側面加以多區 計’能將同一視角之光線由分佈於不同 避免整片之亮面造成視覺上之不舒適， 光線更加均勻。 唯，以上所述者，僅為本創作之較 已並非用以限定本創作實施之範圍， 式亦皆在本案的範疇之中；故此等熟習 出等效或輕易的變化者，在不脫離本創 範圍下所作之均等變化與修冑，皆應涵 之專利範圍内。 效將進入透 因為發光二· 落差，使得 而於入光面 ，且便利且 出光之均勻 咸反射之設 區域提供， 使得照明之 佳貫施例而 其他轉變方 此技術所作 作之精神與 蓋於本創作 16 M432143 【圖式簡單說明】 第1圖，為本創作第一實施例之立體外觀圖。 第2a圖，為本創作第一實施例之剖面示意圖。 第 2b圖，為本創作第一實施例其他態樣剖面圖 (一）。 第 2c圖，為本創作第一實施例其他態樣剖面圖 第 2d圖，為本創作第一實施例其他態樣剖面圖Out, avoid creating a large area of bright areas. The multi-region reflective structure 84 is a plurality of mesh structures 8401. In this embodiment, each of the mesh structures 840 1 is another hexagonal shape that is adjacent to each other to become a feather-like shape. Deploying to the bottom of the cone, and the side of each of the grid structures 840 1 is a straight line or a smooth curve. When the light-emitting diode light source 4′′ is low in brightness or composed of two or more light-emitting diodes, The light diverging from the light-emitting diode light source 4" is not concentrated on a bright spot, so the central region of the mother must provide a astigmatism structure to illuminate the curved or straight line of the multi-region reflective structure 84 in the mesh structure 84〇1. The edges create reflections that spread the light to different viewing angles, avoiding the situation where the single-view produces a bright area. In order to reduce the amount of light refracting the body 8 from the optical curved surface 84, the amount of light reflected to the light-emitting surface 82 is increased. The improved structure of the light-emitting diode lens further includes a reflective layer 86 disposed outside the body 1 and The optical curved surface 84 and the mesh structure 84〇1 are coated with a material having a high reflectivity such as metal, PP or PET, thereby increasing the amount of light to enhance the brightness. 15 M432143 In summary, in the implementation of this creation, the light of the mirror can be refracted to different angles, which greatly reduces the high brightness of the polar point source and the illumination of the edge. The light emitted by the lens exhibits uniform brightness over the entire surface. The converging design not only effectively improves the angle of light refraction, but also has a significant effect. The multi-zone of the side of the lens can make the light of the same viewing angle be visually uncomfortable by distributing the different bright surfaces of the whole film, and the light is more uniform. However, the above-mentioned ones are only for the purpose of limiting the scope of this creation, and are also within the scope of this case; therefore, those who are familiar with equivalent or easy changes, without departing from this The equal changes and repairs made under the scope of the creation shall be within the scope of the patent. The effect will be provided by the light-emitting surface, which is provided on the light-incident surface, and is provided in a convenient and uniform salt-reflecting area, so that the illumination is better and the other transformations are made by the spirit of the technology. This creation 16 M432143 [Simple description of the drawing] Fig. 1 is a perspective view of the first embodiment of the creation. Fig. 2a is a schematic cross-sectional view showing the first embodiment of the creation. Fig. 2b is a cross-sectional view (1) of another aspect of the first embodiment of the creation. 2c is a cross-sectional view of another aspect of the first embodiment of the creation, and FIG. 2d is a cross-sectional view showing another aspect of the first embodiment of the creation.
I ° 第3a圖，為本創作多區域反射結構示意圖（一）。 第3b圖，為本創作多區域反射結構示意圖（二）。 第4圖，為本創作第二實施例之立體外觀圖。 第5圖，為本創作第二實施例之剖面示意圖。 第6圖，為本創作之使用示意圖。 第7a圖，為本創作第三實施例之立體外觀圖。 第7b圖，為本創作第三實施例之剖面示意圖。 第8a圖，為本創作第四實施例之立體外觀圖。 第8b圖，為本創作第四實施例之剖面示意圖。 【主要元件符號說明】 1 ' 7 > 8 10 ' 70 ' 80 100 12 ' 72 ' 82 本體 入光面 第一發散點 出光面 17 M432143 120 、 720 14 ' 74 、 84 140 ' 740 、 840 1401 ' 7401 ' 8401 16' 76 ' 86 2 ' 2， 、 2" 3 4 、 4， 、 4" 第二發散點 光學曲面 多區域反射結構 網格結構 反射層 中央軸心線 安裝構件 發光二極體光源 18I ° Fig. 3a is a schematic diagram of the multi-region reflection structure of the creation (1). Figure 3b is a schematic diagram of the multi-region reflection structure of the creation (2). Fig. 4 is a perspective view showing the second embodiment of the creation. Fig. 5 is a schematic cross-sectional view showing a second embodiment of the creation. Figure 6 is a schematic diagram of the use of this creation. Figure 7a is a perspective view of the third embodiment of the creation. Figure 7b is a schematic cross-sectional view showing a third embodiment of the creation. Figure 8a is a perspective view of the fourth embodiment of the creation. Figure 8b is a schematic cross-sectional view showing a fourth embodiment of the present invention. [Description of main component symbols] 1 ' 7 > 8 10 ' 70 ' 80 100 12 ' 72 ' 82 The first divergent point of the body into the light surface 17 M432143 120 , 720 14 ' 74 , 84 140 ' 740 , 840 1401 ' 7401 ' 8401 16' 76 ' 86 2 ' 2, , 2" 3 4 , 4, 4" Second divergence point optical surface multi-region reflection structure Grid structure Reflection layer Central axis line mounting member Light-emitting diode source 18